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A_N^{\rm pref}
=\frac{\epsilon_N^\star}{L-\mu}
\left(4N^2+16\sum_{m=1}^{N-1}m^2\right)^{1/2}
=\frac4{\sqrt3}\frac{N^{3/2}}{L-\mu}\epsilon_N^\star(1+o(1)), $$ and this is sharp in the causal two-term class with Chebyshev exactness at every prefix. For terminal-only exactness, Jacobi coordinates give $P_N=2^{1-N}T_N$: the spectrum is fixed at the midpoint Chebyshev nodes, while the spectral weights parametrize the realizations. The sine weights give a final-exact Jacobi method with the same terminal residual and $$
A_N(J_N^{\sin})
=2\sqrt{c_{\sin}}\frac{N^{3/2}}{L-\mu}\epsilon_N^\star(1+o(1)),
\; 2\sqrt{c_{\sin}}\approx2.137936<4/\sqrt3. $$ Thus the Chebyshev terminal polynomial does not determine the first-order Hessian-drift gain. The experiments show the finite-horizon effect: lower stochastic curvature overhead, larger admissible-block frontiers, accurate time-varying quadratic predictions, and lower restart cost on an endpoint-coupled smooth strongly convex GLM.
From: Dmitry A. Pasechnyuk [view email]
[v1]
Mon, 15 Jun 2026 13:05:17 UTC (428 KB)
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